Disk reproducing speed control method and a disk reproducing apparatus using this method

ABSTRACT

When a deviated gravity disc is reproduced at a higher rate with the disc reproducing apparatus, an excessive vibration is generated and this vibration gives adverse effect on the disc reproducing apparatus and peripheral components/apparatuses, and/or may represent an annoyance to a user. A vibration information detector for detecting vibration of the disc reproducing apparatus or a deviated gravity information detector for detecting amount of gravity deviation of disc is provided, and as a result of such detection of an imbalance (i.e., excessive vibration or mass eccentricity), and a reproducing rate switching control controls sets and limits the reproducing rate of the disc reproducing apparatus to a substitute speed which is lower or higher than a normal reproducing speed.

CROSS-REFERENCE TO RELATED APPLICATIONS

This application is a continuation of U.S. Ser. No. 08 899,335 filedJul. 23 1997, now U.S. Pat. No. 6,351,440.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention generally relates to a disc reproducing method andapparatus which utilize a disc motor for rotating a disc and an opticalpickup to realize high speed reproduction, and more particularly relatesto a disc reproducing method and apparatus which are suitable forprevention of excessive oscillation and/or vibration in a radialdirection of a disc during high speed rotation resulting from animbalance (e.g., disc eccentricity imbalance, mass imbalance, etc.).

2. Description of Related Art

Use of a so-called compact disc-read only memory (CD-ROM) apparatus(utilizing CD-ROM's as recording/reproduction medium) as a peripheraldevice of a personal computer has gained in popularity and frequency inrecent years. Since introduction, whereupon the CD-ROM apparatus wasstandardized to operate at a predetermined 1X speed or rate, technologyhas advanced tremendously, leading to ever increasing operating speedsfor the CD-ROM apparatus, i.e., for realization of higher speed datatransfer rates. Recently, an 8X speed (i.e., 8 times the originalstandardized 1X speed) is commonplace, and it is now estimated that highspeed data transfer of a 12X speed or higher will become commonplace inthe near future.

For background discussion, FIG. 7 shows a schematic basic block diagramof a servo system used for disc motor control of a disc reproducingapparatus. More particularly, the FIG. 7 arrangement may be dedicated toreproduce only CD-ROMs on which the information of a computer(hereinafter called CD-ROM information) is recorded, or may also be ableto reproduce CDs on which audio information is recorded. If the disc 1is a CD, the rotational speed is uniquely defined, however, if the disc1 is a CD-ROM, for example, it can be reproduced at a multiplicity ofdifferent speeds, e.g, X times as high as a standardized rotationalspeed of 1.2 m/sec. More particularly, as described above, recentlyreproduction at an 8X or 12X rate is mainstream.

Within FIG. 7, the information reader 4 (i.e., head arrangementincluding a laser, lenses, sliders, actuators, etc.) convertsinformation recorded on a disc 1 into an electrical signal and theninputs the signal to a demodulating circuit 6. The demodulating circuit6 demodulates the electrical signal and a signal processing circuit 7generates a clock signal from the demodulated signal. A disc motor servocircuit 8 controls the rotating speed of a disc motor 2 via the discmotor driving circuit 3 so that the clock signal becomes equal to areference clock signal generated by a reference clock generating circuit9.

FIG. 8 shows relationship between a disc reproducing rate multiplicationratio according to a reproducing position and a disc rotating speed. Therecording/reproducing system of this exemplary CD-ROM is a constantlinear velocity (CLV) system in which linear speed is set to a constantvalue. In this system, a rotating speed of the disc changes depending ona current reproducing position of the head on the disc. In suchdiscussed CLV system, since a reference rotating speed is 1.2 m/sec in astandard reproducing rate (i.e., in a 1X original standard speed) and asignal recording area of a disc is within a disc region from 25 mm to 58mm in a radius direction from a center of the disc, for a 4X (i.e.,4-fold) reproducing operation, the rotating speed (frequency) at aninnermost position of the 25 mm radius is about 32 Hz as can be seenfrom the characteristic curve 30 in FIG. 8. Similarly, in an 8X (i.e.,8-fold) reproducing operation, the maximum rotating speed is about 64 Hzas can be seen from the characteristic curve 31, and in the 12X (i.e.,12-fold) reproducing operation, the maximum rotating speed is about 96Hz as can be seen from the characteristic curve 32.

Turning discussion now to FIG. 9, at times, a certain disc 1 which isloaded into and attempted to be reproduced (i.e., read) by a discreproducing apparatus may have a center of rotation 33 (which is thecenter of disc 1) which is deviated from a center of gravity or centerof mass point 34. Such disc situation is hereinafter called a deviatedgravity disc. Such deviated gravity disc may be generated duringmanufacturing, for example, because a disc material pressure is uneven,an unbalanced paint distribution is applied to a surface of the disc, orby reason that an index label is attached on the disc surface aftermanufacturing thereby to imbalance the disc. When this deviated gravitydisc 1 is rotated around the center 33, a force indicated by a forcevector 35 is generated at the point 33, in a direction of the point 34.Therefore, when this deviated gravity disc 1 is reproduced by the discreproducing apparatus, the force 35 works on the disc, disc clamp/mountand disc motor during rotation to fling the disc side to side, andvibration may be generated in a direction matching a major plane of thedisc reproducing apparatus. Such situation is called a mass eccentricdisc.

The above-mentioned force 35 increases in proportion to a square of thedisc rotating speed. Namely, during a reproducing operation in the 8Xreproducing rate, a force equal to 4 times that in the 4X reproducingrate is generated, and during a reproducing operation in the 12Xreproducing rate, a force equal to 9 times that of the 4X reproducingrate is generated. Therefore, with improvement in a disc reproducingrate (i.e., rotating speed) of the disc reproducing apparatus, vibrationgenerated when a deviated gravity disc is reproduced becomes large. Suchvibration can result in a failure of operation (e.g., burn out,misreading, etc.) of the disc reproducing apparatus, can have an adverseeffect on components installed in close proximity to the vibrating disc,a noise generated therefrom can be an annoyance to a user, and/orvibration can cause the disc reproducing apparatus to move across asurface on which it is placed.

The above-discussed vibration phenomenon is due to a mass eccentricityimbalance of the disc, causable (i.e., presently causing or capable ofcausing) of at least one of a radial oscillation and radial vibrationabove a predetermined rotational speed, i.e., oscillation/vibrationdirected along a radial direction (i.e., in a major plane) of the discso as to cause a disc to fling side-to-side as the disc is rotated. Suchmass eccentricity imbalance is the imbalance of most interest in thepresent invention. Another imbalance of interest to a smaller degree isa centering eccentricity imbalance, i.e., a centering eccentricityimbalance of the disc, causable of at least one of a radial oscillationand radial vibration above a predetermined rotational speed, i.e.,oscillation/vibration directed along a radial direction (i.e., in amajor plane) of the disc so as to cause a disc to fling side-to-side asthe disc is rotated. Centering eccentricity imbalance results, forexample, when a disc is loaded with its disc center misaligned to acenter of a rotator arrangement (i.e., rotating motor, disc mount/clamp,etc.). Misalignment may be due to sloppy loading of the disc to themount/clamp, excessively sized central mounting hole in the disc,excessively small or worn mount/clamp, etc. Centering eccentricityimbalance affects oscillation/vibration and operation of the discreproducing apparatus to a lesser degree than that of mass eccentricityimbalance. However, the principles and arrangements of the presentinvention are equally applicable to centering eccentricity imbalance asmass eccentricity imbalance.

Continuing in discussion, FIG. 14 is a block diagram showing anotherCD/CD-ROM disc reproducer arrangement, and in greater detail. Moreparticularly, a reference number 1 denotes a disc, T denotes a track ortracks, L denotes a beam (e.g., laser beam), 2 denotes a disc motor, 3denotes a disc motor driver or control circuit, 4 denotes a headarrangement or information reader, 40 denotes a preamplifier circuit, 5denotes a tracking driver or control circuit, 7 denotes a signalprocessing circuit, 50 denotes a CPU, 10 denotes an audio circuit, 11denotes an audio signal output terminal, 12 denotes a CD-ROM decoder and13 denotes a CD-ROM signal output terminal. More particularly, the FIG.14 arrangement can be used to reproduce both CDs and CD-ROMs as wasdiscussed above with respect to the arrangement of FIG. 7. CPU 50receives a request along an input line I from an external device such asa host computer, issues an instruction A for rotational speed to a discmotor control circuit 3 in response to this request, and sets therotational speed of the disc 1 to a speed requested from the externaldevice.

Helical or concentric tracks T where information is recorded are formedon the disc 1, and an information reader 4 reads audio information orCD-ROM information from any selected track T by radiating a beam L(e.g., a laser beam) on this track T and outputs reflected readinformation as a read signal. After this read signal is amplified andthe waveform is shaped by a preamplifier circuit 40, the signal issupplied to a signal processing circuit 7, and predetermined processingis applied to the signal. More particularly, if the read signal is anaudio information signal, the signal is further processed in an audiocircuit 10, or if the read signal is a CD-ROM information signal, it isprocessed in a CD ROM decoder 12, and output from output terminals 11and 13, respectively.

The head arrangement or information reader 4 may be constituted bylaser, lenses, a pickup, a main actuator/slider for coarsely moving thepickup for major distances (i.e., across tracks) in the radial directionof the disc 1, a minor actuator/slider for finely moving the pickup forminor distances (i.e., precisely aligning to a particular track) in theradial direction of the disc 1, a focusing actuator/slider for focusingthe laser beam L onto a track surface of the disc, and may haveadditional components. A beam L from the pickup can sequentially radiatea series of tracks T owing to movement of the actuators/sliders as thedisc 1 is rotated. The disc reproducer is further provided with atracking control circuit 5 for controlling a position of this condenserin the direction of the width of the track T so as to let a beam Lfollow the track T, and other components. A part of a read signalamplified by the preamplifier circuit 40 is supplied to a trackingdriver or control circuit 5. This tracking control circuit 5 detects astate in which a beam L is following the track T based upon the suppliedread signal and generates a tracking control signal B according to theresult of detection. The tracking control of the pickup of theinformation reader 4 is controlled by this tracking control signal B sothat a beam L always precisely follows the track T.

To access a desired track T, CPU 50 outputs an inhibiting signal C tostop the operation of the tracking control circuit 5 so that a trackingcontrol signal B is prevented from being output and moves the pickup ofthe information reader 4 in the radial direction of the disc 1 at highspeed by the slider so that a beam L is radiated upon this desired trackT. This allows a beam L to cross plural tracks causing a read signaloutputted from the information reader 4 to be a pulse signal having anamplitude which fluctuates or pulses every time the beam L crosses atrack, which pulse signal is called a track crossing pulse hereafter.The track crossing pulse D is detected by and supplied from thepreamplifier circuit 40 to CPU 50. CPU 50 recognizes the number oftracks which the beam L crosses by counting a number of track crossingpulses D and determines whether a beam L has reached a desired track ornot.

When the tracking control circuit 5 supplies a tracking control signal Bto the information reader 4, the tracking control arrangement iscontrolled and a beam L follows the track T with the pickuptheoretically stopped opposing a desired track in this informationreader 4. However, in practice stopping the pickup opposed to a desiredtrack may not be practical because a track location may oscillate (dueto eccentricity as described above and below) and because there is alimit in the quantity of displacement (fine adjustment) of a beam L bythe tracking arrangement. Accordingly, in a practical situation, thepickup is typically adjustingly moved in the radial direction of thedisc by the actuators/sliders and tracking arrangement periodically,i.e., the pickup is intermittently moved in the radial direction of thedisc 1.

If such a mass eccentric disc is rotated at a low rotational speed, forexample, a 1X speed, oscillation may hardly occur because rotationalspeed is slow. However, when rotational speed is increased to a highrotational speed, for example 8X or 12X (in order to accomplish highspeed reproduction), the disc reproducer may experienceoscillation/vibration and track eccentricity in a direction parallel toa major plane of the disc. More particularly, oscillation/vibration andtrack eccentricity may be only experienced or increased as rotationalspeed is increased. For track eccentricity below a predetermined value,tracking control and track following can still be accomplished, but ifabove the predetermined value, tracking control and track followingcannot be accomplished. Though it varies depending upon the quantity ofmass eccentricity, according to experiments, when reproduction isexecuted at approximately a 6X rate or more, oscillation/vibration,track eccentricity and noise occurs. Therefore, in the case ofreproduction of a mass eccentric disc at an 8X rate which is the recentmainstream, a large oscillation/vibration, track eccentricity and noiseare generated by the disc reproducer, undesirable oscillation may beapplied to components installed in close proximity to the disc, and suchoscillation may have a detrimental effect upon components of and workaround this disc reproducer.

As an example of a detrimental effect on a particular component, in apickup, a condenser is normally held by an elastic member and theposition of this condenser is controlled according to a tracking controlsignal supplied to tracking arrangement so that a beam follows (that is,tracks) a track. However, when this tracking control is stopped, thecondenser held by the elastic member is oscillated by and insynchronization with the disc imbalance vibration. When a discreproducer is oscillated by the rotation of a mass eccentric disc at lowrotational speeds, the free condenser is oscillated slightly at the samephase as this disc reproducer because the disc oscillation is small.However, when the rotational speed of the disc is increased, theamplitude/frequency of oscillation generated in the disc reproducer isincreased, and the condenser is oscillated at a frequency according tothe transfer function proper to the elastic member holding thecondenser.

SUMMARY OF THE INVENTION

This invention is directed toward satisfying the aforementionedimbalance and oscillation/vibration problems in reproduction of a disc.More particularly, it is an object of the present invention to provide adisc reproducing method and apparatus which assure higher reliabilityand safety in operation by preventing an excessive oscillation/vibrationgenerated during rotation of an imbalanced disc.

As explained above, when an imbalanced disc is rotated/reproduced athigh reproduction rates (e.g., 8X, 12X), vibration becomes large. Inorder to combat such problem, when an imbalance vibration is generatedand encountered during high speed reproduction at a predeterminedrotational speed, vibration can be lowered by reducing and/or increasingthe rotational speed (i.e., reproduction rate). More particularly, alowering of rotational speed substantially lowers an imbalance force(vector 35; FIG. 9), thereby to eliminate the generation of vibration.In contrast, a raising of rotational speed will eventually reach asituation where a mass of the disc, disc/clamp, motor shaft, etc. is toogreat to move fast enough to follow the high rotational frequency of theimbalance force (vector 35; FIG. 9), thereby avoiding vibration.

Moreover, in order to attain the objects explained above, according tothe disc reproducing method of the present invention, informationindicating an imbalance (e.g., deviated gravity, eccentricity) of thedisc is detected and when smaller than a predetermined value, a discreproducing operation is performed at a first reproducing rate, and whenlarger, the disc reproducing operation is performed at a secondreproducing rate which is lower than the first reproducing rate.

Therefore, in view of achieving the objects explained above, accordingto one disc reproducing method and apparatus of the present invention,information about vibration of the disc reproducing apparatus isdetected, and when such information indicates a level of vibrationsmaller than a predetermined value, disc reproducing operation isperformed at a normal reproducing rate, and when such informationindicates vibration larger than the predetermined value, a discreproducing operation is performed at a substitute reproducing ratewhich is different (i.e., lowered or raised) from the normal reproducingrate.

In addition, the disc reproducing apparatus of the present inventioncomprises, in view of achieving the object explained above, a switchingcontroller for controlling the switching of the disc reproducing rate tothe first reproducing rate or the second reproducing rate (i.e., higheror lower second reproducing rate), so as to control the disc reproducingrate to the first reproducing rate when a detected signal from thevibration information detector is smaller than the predetermined value,and to the second reproducing rate when the detected signal is largerthan the predetermined value.

Moreover, the disc reproducing apparatus of the present inventionfurther can comprise, in order to achieve the object explained above, adeviated gravity information detector for detecting information about adeviated gravity of a disc, and a switching controller for controllingswitching of the disc reproducing rate to the first reproducing rate orto second reproducing rate which is lower than the first reproducingrate, i.e., to set the disc reproducing rate to the first reproducingrate when the detected signal from the deviated gravity informationdetector is smaller than the predetermined value and to the secondreproducing rate when the detected signal is larger than thepredetermined value.

In addition, the present invention also comprises a display so that auser can confirm a present state of the arrangement, i.e., as to whetheror not an imbalanced condition has been detected, and/or as to whetheror not the disc reproducing rate is switched to the second reproducingrate from the first reproducing rate. Construction according to thepresent invention enables high speed reproduction, for example , of a12X (i.e., 12-fold) rate when gravity deviation of disc is judged to besmall or when vibration is sufficiently small so as not to represent anyproblem even under a high reproduction rate, and also enables automaticswitching of the disc reproducing rate to an appropriate changed ratedepending on a degree of gravity deviation or vibration. Moreparticularly, automatic switching can be provided to switch from anormal desirable 12X speed to a differing (i.e., lower or higher) speed,for example, an 8X speed or 4X speed under control by the switchingcontroller when gravity deviation of disc is judged to be large or whenvibration is generated under a present reproduction rate.

Alternative to dynamic detection, a static detection arrangement can beused wherein the quantity of mass eccentricity of a disc which isequivalent to the quantity of displacement between the center of gravityof the disc and the center point of the disc is detected beforehand toautomatically warn or inhibit reproduction of the mass eccentric disc athigh speed.

In accomplishing the above objects, however, provision of requireddetectors for detecting the oscillation of a disc reproducer, fordetecting the quantity of mass eccentricity of a disc and others do nothave to be provided by additional components added to a disc reproducer,i.e., the number of parts, scale and cost of circuits/arrangements of adisc reproducer do not have to be increased as the present invention canbe implemented with components already present in disc reproducingapparatus. More particularly, another specific object of the presentinvention is to provide a mass eccentric disc detecting method whichenables detecting the quantity of mass eccentricity of a disc preciselywithout or only minimally adding equipment to a disc reproducerarrangement.

A further object is to provide a disc reproducer which can provideautomatic control so that if the disc is a mass eccentric disc, therotational speed of the disc is made optimum according to a quantity ofmass eccentricity.

To achieve the above object, according to the present invention, a discis rotated at first rotational speed and at second rotational speedwhich is faster than the first rotational speed with tracking controlstopped, a track crossing signal which is a pulse every time a beamcrosses a track on a disc is obtained at differing rotational speeds andthe information of the quantity of mass eccentricity of a disc isdetected based upon a comparison of track crossing counts at first andsecond rotational speeds.

As force generating oscillation due to the rotation of a mass eccentricdisc is in proportion to the square of the rotational speed of this discand the quantity of mass eccentricity of the disc, the oscillation of adisc reproducer is increased in proportion to the rotational speed ofthe disc, and if the above first rotational speed is slow rotationalspeed to the extent that the disc reproducer is hardly oscillated andthe above second rotational speed is high rotational speed at which thedisc reproducer is oscillated when a mass eccentric disc is rotated atthe rate, in the case of the former the scanning trace of a beam on thedisc forms substantially circular trace 90 shown by a dotted line inFIG. 15, however, in the case of the latter, when the condenser isoscillated at the frequency proper to the elastic member holding thecondenser, for example the scanning trace forms oval trace 92 shown by abroken line in FIG. 15 because tracking control is not executed and thecondenser is free.

If the circular trace 90 and the oval trace 92 are compared, in the caseof the former the trace 90 is substantially along a track T because thetrack T is helical or circular and in the case of the latter, moretracks are crossed, a read signal obtained from a pickup is a pulsesignal the frequency of which is high or the shortest cycle of which isshort. Therefore, information showing the degree of the masseccentricity of a disc can be obtained based upon the difference betweenboth described above.

For a concrete method of detecting the information of the quantity ofmass eccentricity of a disc according to the present invention, thenumber of the above pulse signals, that is, track crossing signals atthe predetermined number of revolutions is counted or the cycle of thistrack crossing signal is detected and the above number of pulses, theratio or the difference of a cycle at the above first and secondrotational speed are obtained. The ratio or difference shows the degreeof mass eccentricity of a disc.

According to the present invention, it is determined whether the disc isa mass eccentric disc or not based upon the quantity of masseccentricity detected as described above and the allowable maximumrotational speed of a disc is limited according to the detected quantityof mass eccentricity. Hereby, in a disc reproducer, oscillation can beprevented from being caused.

Further, according to the present invention, the information of thedetected quantity of mass eccentricity is displayed on display to letthe outside know whether an installed disc is a mass eccentric disc ornot.

The foregoing and other objects, advantages, manner of operation, novelfeatures and a better understanding of the present invention will becomeapparent from the following detailed description of the preferredembodiments and claims when read in connection with the accompanyingdrawings, all forming a part of the disclosure hereof this invention.While the foregoing and following written and illustrated disclosurefocuses on disclosing embodiments of the invention which are consideredpreferred embodiments at the time the patent application was filed inorder to teach one skilled in the art to make and use the invention, itshould be clearly understood that the same is by way of illustration andexample only and is not to be taken by way of limitation, the spirit andscope of the present invention being limited only by the terms of theappended claims.

BRIEF DESCRIPTION OF THE DRAWING(S)

The following represents brief descriptions of the drawings, wherein:

FIG. 1 is a block diagram of an exemplary disc reproducing apparatus ofa first embodiment of the present invention.

FIG. 2 is a block diagram showing an exemplary structure of a vibrationdetector arrangement of the present invention.

FIG. 3 is a block diagram of an exemplary disc reproducing apparatus ofa second embodiment of the present invention.

FIG. 4 is a block diagram showing an exemplary structure of a deviatedgravity detector arrangement of the present invention.

FIG. 5 is a diagram showing an exemplary layout pattern/positioning ofweight detectors in an embodiment of the present invention.

FIG. 6 is a block diagram showing another exemplary structure of adeviated gravity detector arrangement of the present invention.

FIG. 7 is a schematic basic block diagram of a background servo systemof a disc motor control of the disc reproducing apparatus, forbackground discussion.

FIG. 8 is a diagram showing a background relationship between a discreproducing rate multiplication ratio and a disc rotating speed, againfor background discussion.

FIG. 9 is a diagram showing a force generated during rotation of adeviated gravity disc, further for background discussion.

FIG. 10 is a block diagram showing a first embodiment of a masseccentric disc detecting method and a disc reproducer according to thepresent invention.

FIG. 11 shows a graph showing the characteristics of the number of trackcrossing pulses per rotation of a disc for the rotational speed of thedisc.

FIG. 12 is a block diagram showing a second embodiment of the masseccentric disc detecting method and the disc reproducer according to thepresent invention.

FIG. 13 shows a waveform which example of a track crossing pulse.

FIG. 14 is a block diagram showing an example of a conventional typedisc reproducer.

FIG. 15 shows the scanning trace disc according to the quantity of masseccentricity or a disc when tracking control is not executed.

FIG. 16. illustrates an ideal actuator driving current of a disc withoutand with imbalance.

FIG. 17 showing ideal actuator temperature of a disc without and withimbalance.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS OF THE INVENTION

Before beginning a detailed description of the subject invention,mention of the following is in order:

When appropriate, like reference numerals and characters are used todesignate identical, corresponding or similar components in differingfigure drawings.

In the description of the preferred embodiments, numeric values areconcretely shown; however, such numeric values are only for convenienceof description and the present invention is not limited thereto.

Turning now to detailed description of the invention, FIG. 1 is a blockdiagram of a disc reproducing apparatus according to a first embodimentof the present invention. More particularly, in FIG. 1: referencenumeral 1 designates a disc; 2, a disc motor; 3, a disc motor drivingcircuit; 4, an information reader (i.e., head assembly) comprising atransfer arrangement; 5, a transfer driving circuit for controlling anddriving the transfer arrangement of the information reader 4; 6, ademodulating circuit for demodulating signals from the informationreader 4; 7, a signal processing circuit; 8, a disc motor servo circuit;9, a reference clock generating circuit; 10, an audio circuit; 11, anaudio output terminal; 12, a CD-ROM decoder, 13, a CD-ROM signal outputterminal; 14, a vibration detector for detecting vibration of the discreproducing apparatus; 15, a vibration identifier; 16, a reproducingrate switching controller comprising a frequency dividing circuit fordividing the frequency of the reference clock signal outputted from thereference clock generating circuit 9, and a control circuit forcontrolling the dividing ratio of the frequency dividing circuit. Inthis FIG. 1, an audio circuit and CD-ROM decoder, etc. are also shown,although these are not directly related to the subject matter of thepresent invention.

When a deviated gravity disc having a gravity (mass) point deviated fromthe center of the disc is reproduced by the disc reproducing apparatusat the higher rate such as a 12X rate, vibration is generated in thedisc reproducing apparatus. Vibration gives influence to the informationreader 4, but when this influence is within an acceptable range whichcan be compensated/controlled by the transfer control circuit 5 and discmotor control circuit 8, the information reader 4 converts theinformation of disc 1 into an electrical signal. This electrical signalis further processed by the demodulating circuit 6, signal processingcircuit 7, audio circuit 10 or CD-ROM decoder 12 and the signal isfinally outputted from the audio output terminal 11 or CD-ROM signaloutput terminal 13. However, if vibration is large, operation of thedisc reproducing apparatus may be adversely affected (e.g., operateerroneously), and/or be an annoyance to a user.

The vibration detector 14 detects vibration of the disc reproducingapparatus and outputs a signal depending on an amplitude of vibration.This vibration detector 14 is constructed, for example, using an impactvoltage converting element, centrifugal force detector, etc. Thevibration identifier 15 identifies an output signal of the vibrationdetector 14, judges whether or not the vibration of the disc reproducingapparatus is sufficiently large to exceed the predetermined value, andif sufficiently large, outputs a control signal to the reproducing rateswitching control 16 to reduce the reproducing rate. Responsive to suchcontrol signal, the reproducing rate switching control 16 generates afrequency-divided clock signal by dividing the reference clock signaloutputted from the reference crock generating circuit 9 with a dividingratio which depends on the control signal from the vibration identifier15, and then outputs this frequency-divided clock signal to the discmotor servo circuit 8. The disc motor servo circuit 8 controls therotating speed of the disc motor 2 via the disc motor driving circuit 3so that the frequency-divided clock signal matches the clock signaloutputted from the signal processing circuit 7. Therefore, the rotatingspeed of the disc motor 2 is reduced depending on the control signaloutputted from the vibration identifier 15.

As mentioned above, a force generated during rotation of the deviatedgravity disc which causes vibration of the disc reproducing apparatus isproportional to square of the rotating speed. Therefore, when thereproducing rate of the deviated gravity disc is lowered to a 4X rate,for example, from a 12X rate, the rotating speed is reduced to ⅓of the12X rate and thereby the force available for causing vibration isreduced to {fraction (1/9)}. Accordingly the vibration of the discreproducing apparatus can be reduced.

Turning next to FIG. 2, disclosed is an embodiment of a detectorarrangement for detecting information about vibration of the discreproducing apparatus using a control signal outputted from thetransfer/tracking driving arrangement (in place of the vibrationdetector 4). In FIG. 2, reference numeral 17 designates a referencesignal generator which outputs a reference signal which is equal to thecontrol signal outputted from the transfer/tracking driving arrangementwhen an ideal disc not including any deviated gravity is reproduced.Reference numeral 18 indicates a comparator. When vibration is generatedin the disc reproducing apparatus by reproduction of the deviatedgravity disc at, a higher rate (e.g., 12X), a disturbance is generatedin a control signal outputted from the transfer/tracking drivingarrangement, a degree of such disturbance depending on an amplitude ofvibration. The reference signal generator 17 outputs the referencesignal which is identical to an ideal control signal, namely a controlsignal not including any disturbance, i.e., similar or identical to asignal which would be outputted by the transfer/tracking drivingarrangement when an ideal disc not including any deviated gravity isreproduced at such higher rate. The control signal outputted from thetransfer/tracking driving arrangement can be either of a driving currentor driving voltage of any actuator arrangement within the informationreader (i.e., continued oscillatory tracking by an actuator will causeabnormal current or voltage fluctuations), for example, FIG. 16illustrates an ideal driving current 100 of a disc without imbalance,and an irregular driving current 102 of a disc with imbalance. Ameasured actuator temperature parameter can also be used (i.e.,continued oscillatory tracking by an actuator will generate additionalheat as the actuator is having to work harder), with FIG. 17 showingidea temperature 100 of a disc without imbalance, and an irregulartemperature 112 of a disc with imbalance.

Continuing with the description, the reference control signal and theactual control signal (which includes the disturbance due to vibration)are compared with each other in the comparator 18 to detect a level ofdisturbance of the control signal. Accordingly, suchdescription/illustration shows that it is possible to detect informationabout vibration of the disc reproducing apparatus using the controlsignal outputted from the transfer driving circuit 5 (i.e., without theaddition of separate detector components). As another arrangement whichcan detect imbalance without the addition of separate detectors, sincedisturbance of a control signal due to vibration is also generated inthe control signal outputted from the disc motor servo circuit 8 of FIG.1, it is also possible to detect information about vibration of the discreproducing apparatus from the control signal outputted from the discmotor servo circuit 8. More particularly, detection of an irregularityin a spindle motor current, voltage and temperature of motor 2 can alsobe used.

In a dynamic testing approach with the first embodiment explained above,a disc can be initially attempted to be reproduced, for example, at ahigh rate (e.g., 12X), and upon detection of excessive vibration due toa deviated gravity disc, a reproducing rate of disc can be automaticallylowered to reduce the vibration. However, initially assuming a balancecondition and initially operating at a high rate (e.g., 12X) may bedangerous/damaging to users and device components. Accordingly, it maybe preferable for safety considerations to detect deviated gravity ofdisc before operating at the high rate, i.e., to initially check for animbalance condition, and then only authorize activation of a high speedwhen an imbalance condition is not initially indicated.

FIG. 3 shows a second embodiment of the present invention consideringthe above initial low speed approach. More particularly, in FIG. 3, thereference numeral 19 designates a deviated gravity detector fordetecting deviation of gravity of disc 1 and outputting a signaldepending on such amount of gravity deviation, and 20 designates adeviated gravity identifier for identifying an output signal from thedeviated gravity detector 19. Other portions designated by likereference numerals to those in FIG. 1 indicate like components.

The deviated gravity identifier 20 judges, when the output signal fromthe deviated gravity detecting 19 exceeds a predetermined value, that adeviation of gravity of disc 1 is large and outputs a control signal tolimit a reproducing rate to a lower rate. The reproducing rate switchingcontrol 16 limits the dividing ratio of the reference clock signaloutputted from the reference clock generating circuit 9 depending on thecontrol signal from the deviated gravity identifier 20. Therefore, thedisc reproducing apparatus of the second embodiment does not perform thereproducing operation at a higher rate for the disc 1 when the deviatedgravity detector 20 identifies a large deviation of gravity of disc 1.That is, when deviation of gravity of disc 1 is large, the reproducingrate is thus set and limited to a lower rate, and thereby the deviatedgravity disc. 1 is never reproduced at the rate as high as 12-fold rateand generation of vibration can be prevented.

The deviated gravity identifier 19 is realized, for example, by thestructure of FIG. 4. In FIG. 4: 21 to 24 represent weight detectors forconverting weight to a voltage; 25, 26, a subtractors; 27, an adder.Again, portions designated by like reference numerals to those in FIG. 3indicate like components. As shown in FIG. 5, the weight detectors 21 to24 are respectively allocated at equal distances from the center of disc1 on linear axes crossing at a right angle at a center of disc 1. Whenthe disc 1 is placed on the weight detectors 21 to 24, a weight of thedisc 1 is distributed on the weight detectors 21 to 24 and these weighsdetectors 21 to 24 output voltages corresponding to the weight appliedthereto. Pairs of such output voltages are input to the subtractors 25,26. Since the weight detectors 21 to 24 are allocated at the positionsshown in FIG. 5, when gravity deviation of disc 1 is almost zero, anequal weight is applied to the weight detectors 21 to 24. In contrast,when the disc 1 has a certain deviation of gravity, differences aregenerated in the weights applied to the weight detector 21 to 24. It isnoted that the weight detectors 21 to 24 can be used to detect weightimbalance during static testing (i.e., with the disc being stopped) ordynamic testing (i.e., with the disc being rotated).

The subtractor 25 detects a voltage difference outputted from the weightdetectors 21, 23, while the subtractor 26 detects a voltage differenceoutputted from the weight detectors 22, 24. Namely, the subtractor 25detects amount of gravity deviation of disc 1 in the linear direction(i.e., axis) upon which the weight detectors 21, 23 are allocated, whilethe subtractor 26 detects amount of gravity deviation of disc 1 in thelinear direction (i.e., axis) upon which the weight detectors 22, 24 areallocated. The adder 27 adds the output voltages of the subtractors 25,26 and outputs a result to the deviated gravity identifier 20.Therefore, the voltage outputted from the adder 27 corresponds to anamount of gravity deviation of the disc 1, and the amount of gravitydeviation of disc 1 can be detected with the structure shown in FIG. 4.While in the structure of FIG. 4, four weight detectors are used,differing arrangements such as three or more weight detectors can beused, and with such alternative arrangements, an amount of gravitydeviation of disc 1 can also be detected with the same operationprinciple.

Continuing further in discussion, FIG. 6 illustrates an embodiment fordetecting information about a deviated gravity of disc 1 using acomparison of parameters measured at least two differing reproductionspeeds. More particularly, in FIG. 6, reference numerals 28, 29designate control amount stores (i.e., memories or storage arrangements)for storing an amount of control of the transfer arrangement of theinformation reader 4. As described in the first embodiment, when adeviated gravity disc 1 is reproduced at a higher reproduction rate(e.g., 12X), vibration is generated in the disc reproducing apparatusand the transfer driving circuit 5 controls the transfer arrangement ofthe information reader 4 depending on the vibration. Accordingly, beingdirectly related to the vibration, an amount of control changesdepending on a square of the reproducing rate of the deviated gravitydisc 1 and an amount of gravity deviation of disc 1. The control amountstore 28 stores an amount of control of the transfer arrangement of theinformation reader 4 when the disc is reproduced at a lower rate, forexample, at a 1X rate, and a control amount store 29 stores an amount ofcontrol when the disc 1 is reproduced at a higher rate, for example, a4X rate. Here, when the disc 1 almost does not have any deviation ofgravity, the control amount of the control amount stores 28, 29 isequal, but if the disc 1 has a certain amount of gravity deviation, anamount of control during the 4X reproduction as stored in the controlamount store 29 becomes larger than the control amount during the 1Xreproduction as stored in the control amount store 28. Therefore, anamount of gravity deviation of the disc 1 can be detected by comparingthe control amounts stored in the control amount stores 28, 29 using thecomparator 18. Again, as was discussed above with respect to the FIG. 2arrangement, since a difference of a control amount due to thereproducing rate is also generated in the control signal outputted fromthe disc motor servo circuit 8, information about a deviated gravity ofdisc 1 can also be detected by comparing the control signal outputtedfrom the disc motor servo circuit 8 at two (or more) different speeds.

As described above, according to the present invention, a vibration of adisc reproducing apparatus or an amount of gravity deviation of a disccan be automatically detected and the reproducing rate can beautomatically controlled depending on the result of such detection.Namely, when the deviated gravity disc 1 is reproduced at a high ratesuch as 12X and excessive vibration is generated, the reproducing rateis automatically switched from the high 12X rate to, for example, alower 8X or 6X rate which do not result in any vibration problem. Inaddition, when amount of gravity deviation is judged large in comparisonto a previously detected amount of gravity deviation of the disc, a discreproducing operation (i.e., data reading) is started only after thereproducing rate has been automatically switched from the 12X rate tothe 8X or 6X rate depending on the amount of gravity deviation.Therefore, operation failure of the disc reproducing apparatus andadverse effects on other apparatus installed in the vicinity thereof,resulting from vibration generated during reproduction of a gravitydeviated disc at a higher reproducing rate, can be prevented.

FIG. 10 is a block diagram showing another embodiment of a masseccentric disc detecting method and a disc reproducer according to thepresent invention. Within FIGS. 10-13, like reference numerals are usedto designate like components from previously discussed Figs. A referencenumber 60 denotes a counter, 62 and 64 denote storage cells, 66 denotesa comparing circuit. As shown in FIG. 10, the counter 60, the storagecells 62 and 64 and the comparing circuit 66 are newly added to thepreviously discussed FIG. 14 disc reproducer, so as to detect theinformation of the quantity of mass eccentricity of a disc 1 using atrack crossing pulse D from a preamplifier circuit 40. Operation of sucharrangement is now described.

More particularly, before reproduction of the information signal isattempted at a high speed, for example, 8X or 12X, CPU 50 issues aninhibiting signal C to stop the operation of a tracking control circuit5, and instructs a disc motor control circuit 3 to initially set therotational speed of the disc 1 to a low speed of approximately a 1X or2X rate, i.e., by issuing an appropriate instruction A. This firstrotational speed is not limited to a 1X or 2X speed, but instead anyspeed which does not cause oscillation/vibration of the disc reproducereven if the disc 1 is a mass eccentric disc, can be used.

When the disc 1 is rotated at the first rotational speed, that is, atslow speed, a signal (e.g., reflected laser beam) is reproduced from thedisc 1 by the information reader 4 and a regenerative signal therefromis amplified by the preamplifier circuit 40 to be waveform shaped. Atleast part of the regenerative signal is supplied to the CPU 50 andcounter 60 as a track crossing pulse D. The CPU 50 uses the trackcrossing pulse D to control access to a desired track T on the disc 1.

In the meantime, the counter 60 counts edges of this track crossingpulse D and is reset by a reset pulse E supplied from the disc motorcontrol circuit 3 at every rotation of the disc 1. Therefore, thecounter 60 can obtain a number N1 of pulses of a track crossing pulse Dfor each rotation of the disc 1, and such count value N1 can be storedin the storage cell 62.

Next, CPU 50 issues an instruction A to rotate the disc 1 at high speedto the disc motor control circuit 3. The rotational speed in this caseis the one (hereinafter called second rotational speed) whichnecessarily oscillates the disc reproducer if this disc 1 is a masseccentric disc, for example, can be an 8X or 12X rate. When the disc isrotated at the second rotational speed, that is, at high speed, asdescribed above, a regenerative signal output from the informationreader 4 and amplified/shaped by the preamplifier circuit 40 is againsupplied to the counter 60 as a track crossing pulse D. The counter 60again counts edges of this track crossing pulse D and is reset by areset pulse E supplied from the disc motor control circuit 3 everyrotation of the disc 1. Therefore, while rotation is conducted at thehigher speed, the counter 60 can obtain a number N2 of pulses of a trackcrossing pulse D and the count value N2 can be stored in the storagecell 64.

As described above, when the number N1 of track crossing pulses when thedisc 1 is rotated at slow speed is stored in the storage cell 62 and thenumber N2 of track crossing pulses when the disc 1 is rotated at highspeed is stored in the storage cell 64, the numbers N1 and N2 of thesepulses can be compared by the comparing circuit 66, and the ratio ordifference of these can be obtained. The result F of such comparison issent to CPU 50.

If the disc 1 is a mass eccentric disc, as described in relation to FIG.15, a scanning trace of a beam L as the disc 1 rotates at low speedforms a substantially circular trace 90, and therefore, no or a verysmall number of track crossings occur so that a small track crossingcount N1 is stored in the storage cell 62. When a mass eccentric disc 1is rotated at the second rotational speed, the scanning trace of a beamL forms a substantially oval trace 92, and therefore, a large number oftrack crossings occur so that a large track crossing count N2 is storedin the storage cell 64. Therefore, the number N2 of track crossingpulses per rotation of the disc 1 stored in the storage cell 64 islarger than the number N1 of track crossing pulses per rotation of thedisc 1 stored in the storage cell 62. Therefore, the ratio N2/N1 (whichis the result F of comparison by the comparing circuit 66) is largerthan 1 or the difference (N2−N1) is positive, and when these values arelarger than a preset threshold value, the disc is decided to be a masseccentric disc.

FIG. 11 graphically shows a change of the number of track crossingpulses per rotation, for various rotational speeds of the disc 1. Moreparticularly, characteristic curve 80 show those of a disc having aquantity of eccentricity and quantity of mass eccentricity which areboth small, i.e., such characteristic curve 80 shows that a number oftrack crossing pulses per rotation of the disc is small and remains at asubstantially small fixed value independent of a change of rotationalspeed. Characteristic curve 82 shows those of a disc having a quantityof eccentricity which is large and a quantity of mass eccentricity whichis small, i.e., such characteristic curve 82 shows that a number oftrack crossing pulses per rotation of the disc 1 is large, and again,the number of track crossing pulses is substantially fixed independentof the change of rotational speed.

Characteristic curve 84 shows those of a disc having a quantity ofeccentricity of which is small and a quantity of mass eccentricity whichis large, i.e., such characteristic curve 84 shows the number of trackcrossing pulses per rotation of the disc is varied as rotational speedis changed. As described above, the number of track crossing pulses isincreased as the rotational speed of the disc is gradually increased andan oscillation frequency generated in the disc reproducer approaches thenatural frequency of the transfer function of an elastic member holdingthe pickup. It is interesting to note that, after rising and reaching amaximum, the number of track crossing pulses then actually decreases asthe rotational speed of the disc is further increased. Such decreasingoscillation/vibration occurs because a frequency generated in the discreproducer moves away from a natural frequency of the transfer functionof rotator arrangement and/or the elastic member holding the pickup,i.e., a mass of the rotator arrangement and/or the pickup is too greatto follow the rotational frequency of the imbalance (eccentricity).

Continuing in discussion, as shown in FIG. 11, f1 is a first rotationalspeed wherein mass eccentricity does not cause vibration or increaseddisc eccentricity along any of the curves 80, 82, 84, and f2 is a secondrotational speed wherein it does. As shown in FIG. 11, it can bedetermined whether the disc 1 is a mass eccentric disc or not bycomparing the number N1 of track crossing pulses stored in the storagecell 62 and corresponding to the first rotational speed f1 and thenumber N2 of track crossing pulses stored in the storage cell 64 andcorresponding to the second rotational speed f2. More particularly, if aresult F of comparison is larger than a preset threshold value, suchresult F functions as information showing the degree of masseccentricity, which the CPU 50 can use to recognize the same.

More specifically, CPU 50 determines whether the currently installeddisc 1 is a mass eccentric disc or not based upon the result F ofcomparison by the comparing circuit 66, and instructs operation at anappropriate reproduction speed. That is, when an result F indicates thata presently installed disc 1 is not a mass eccentric disc, the disc 1 isrotated at a normal rotational speed (e.g., 8X or 12X) according to arequest from an external device. However, if the result indicates thatthe disc 1 is a mass eccentric disc, a maximum rotational speed of thedisc 1 is limited according to the result F, independent or regardlessof a request from an external device. For example, even if the disc 1 isa CD-ROM and high speed reproduction of 8X is requested, the rotationalspeed of the disc is limited to high speed reproduction at a 6X speed orless.

As described above, it can be readily and securely determined whetherthe disc 1 is a mass eccentric disc or not without providing oscillationdetector separately, and with such arrangement, information showing thedegree of the mass eccentricity of the disc 1 can be detected, and themaximum rotational speed can be limited according to the quantity ofmass eccentricity and the disc reproducer can be prevented from beingoscillated.

FIG. 12 is a block diagram showing a second embodiment of a masseccentric disc detecting method and a disc reproducer according to thepresent invention. In discussing new components within such FIG., areference number 70 denotes a shortest cycle detecting circuit. In thisembodiment, the shortest cycle detecting circuit 70 is used in place ofthe counter 60 shown in FIG. 10. A track crossing pulse D is a signalwith a compression waveform as shown in FIG. 13 and a shortest cycle tis determined by the number of track crossing pulses per rotation of adisc and the rotational speed of the disc. Therefore, when therotational speed of the disc 1 is doubled, this shortest cycle t is ½ ifthe number of track crossing pulses per rotation of the disc is notchanged and if the disc reproducer is oscillated and the number of trackcrossing pulses per rotation of the disc 1 is increased, the shortestcycle t is decreased to even smaller than ½.

In the second embodiment shown in FIG. 12, the shortest cycles t1 and t2of a track crossing pulse D for one rotation of the disc 1 are detectedat the respective first rotational speed f1 and the second rotationalspeed f2 by the shortest cycle detecting circuit 70, and such values arestored in storage cells 62 and 64, respectively. In a comparing circuit66, the ratio t1/t2 or difference (t1−t2) between these shortest cyclest1 and t2 are obtained. CPU determines whether the disc 1 is a masseccentric disc or not based upon the result F of such comparison,detects the degree of mass eccentricity and sets the allowable maximumrotational speed of the disc 1 accordingly.

More particularly, if the second rotational speed f2 is ‘n’ times asfast as the first rotational speed f1, the ratio t1/t2 is approximately‘n’ in a case where the disc 1 is not a mass eccentric disc. Thedifference (t₁−t₂) is approximately t₁ (n−1)/n, however, if the disc 1is a mass eccentric disc. If a ratio or difference value exceeds apreset threshold value, it can be determined that the disc is a masseccentric disc and the degree of mass eccentricity can be known from thedegree of the ratio or difference.

The shortest cycle detecting circuit 70 detects each cycle as a countvalue by counting clock pulses of a fixed cycle which occur during, forexample a track crossing pulse D. A first count value which is atemporary shortest cycle and a second count value are compared, and thesmaller count value is set as a new temporary shortest cycle. Every timea count value is obtained, this count value and a count value set as atemporary shortest cycle are compared, and a smaller count value of thetwo is selected and held as a new temporary shortest cycle. Suchoperation is performed for one rotation of the disc 1, and the countvalue of a finally obtained temporary shortest cycle is stored in thestorage cell 62 or 64 as the count value of a true shortest cycle.

As described above, in this second embodiment, the similar effect as inthe above first embodiment can be also obtained.

It should also be apparent that in the embodiment shown in FIG. 10, CPUmay be provided with the function of a circuit consisting of the counter60, the storage cells 62 and 64 and the comparing circuit 66, and in thesecond embodiment shown in FIG. 12, CPU may be also provided with thefunction of a circuit consisting of the shortest cycle detecting circuit70, the storage cells 62 and 64 and the comparing circuit 66. With sucharrangement, circuit configuration is further simplified and device costis reduced.

In addition to the above discussions, a display 68 (FIG. 12) fordisplaying the result of eccentricity determination and/or operationalspeed can be provided, i.e., so as to let a user know the result ofdetection and/or adjustment. For example, for such display 68, agraphical display for displaying information showing whether the disc 1is a mass eccentric disc or not, and information showing allowablemaximum rate reproduction (6X, 4X, 1X) set for the disc 1 can be used.Alternatively, the display can be a simple light emitting diode (LED)indicating when it is determined that the disc is a mass eccentric disc.Other types of indication may also or alternatively be provided, forexample, an audible indicator.

As described above, according to the present invention, the informationof the quantity of mass eccentricity of a disc is detected based uponthe result of comparison by rotating the disc with a tracking controldisabled, and comparing a number of track crossing pulses generated byreading the disc at different rotational speeds. A mass eccentric discis detected without adding new components such as oscillation detector,and therefore, such detection can be precisely performed withoutenlarging the disc reproducer and increasing the cost. As the allowablemaximum rotational speed of a mass eccentric disc is controlledaccording to the detected quantity of mass eccentricity, the discreproducer can be effectively prevented from being oscillated due to amass eccentric disc.

This concludes the description of the preferred embodiments. Althoughthe present invention has been described with reference to a number ofillustrative embodiments thereof, it should be understood that numerousother modifications and embodiments can be devised by those skilled inthe art that will fall within the spirit and scope of the principles ofthis invention. More particularly, reasonable variations andmodifications are possible in the component parts and/or arrangements ofthe subject combination arrangement within the scope of the foregoingdisclosure, the drawings and the appended claims without departing fromthe spirit of the invention, e.g., the following represents anon-exhaustive list of modifications which might readily be apparent toone skilled in the art to which the present invention is directed:

More particularly, the present invention is equally applicable toconstant angular velocity (CAV) arrangements as well as the abovedescribed constant linear velocity (CLV) arrangements. Further, whilethe above description focused mainly on CD and CD-ROM reproducingarrangements, the present invention may be applicable to other types ofarrangements (e.g., CD, CD-ROMs, mini-discs, DVD, etc., including anyother optical disc types which may be introduced in the future), and mayalso be applicable to magnetic disc rotating arrangements.

What is claimed is:
 1. A disc reproducer for rotating a disc,comprising: a detector for detecting vibration of said disc reproduceritself; and a rotator for rotating the disc at a first rotational speedwhich is faster than normal rotational speed; wherein said rotatorrotates the disc at a second rotational speed which is faster than thenormal rotational speed and is slower than the first rotational speedwhen said detector detects the vibration.
 2. A reproducer as claimed inclaim 1, wherein said rotator rotates the disc at the second rotationalspeed when the vibration detected by said detector is larger than apredetermined value.
 3. A reproducer as claimed in claim 2, wherein therotational speed is changed into the second rotational speed in areproducing operation at the first rotational speed.
 4. A reproducer asclaimed in claim 1, wherein said rotator rotates the disc at the secondrotational speed in a reproducing operation at the first rotationalspeed.
 5. A disc reproducer for rotating a disc, comprising: detectingmeans for detecting vibration of said disc reproducer itself; androtating means for rotating the disc at a first rotational speed whichis faster than normal rotational speed; wherein said rotating meansrotates the disc at a second rotational speed which is faster than thenormal rotational speed and is slower than the first rotational speedwhen said detecting means detects the vibration.
 6. A reproducer asclaimed in claim 5, wherein said rotating means rotates the disc at thesecond rotational speed when the vibration detected by said detectingmeans is larger than a predetermined value.
 7. A reproducer as claimedin claim 5, wherein rotational speed is changed into the secondrotational speed in a reproducing operation at the first rotationalspeed.
 8. A method for rotating a disc by a disc reproducer, comprisingthe steps of: detecting vibration of said disc reproducer itself; androtating the disc at a first rotational speed which is faster thannormal rotational speed; wherein the disc is rotated at a secondrotational speed which is faster than the normal rotational speed and isslower than the first rotational speed when the vibration is detected.9. A method as claimed in claim 8, wherein the disc is rotated at thesecond rotational speed when the vibration is larger than apredetermined value.
 10. A method as claimed in claim 8, whereinrotational speed is changed into the second rotational speed in areproducing operation at the first rotational speed.